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A circular loop of wire with radius r = 0.0250 m and resistance R = 0.390 Ω is in a region of the spatially uniform magnetic field, as shown in Fig. E29.23. The magnetic field is directed into the plane of the figure. At t = 0, B = 0. The magnetic field then begins increasing, with B(t) = 0.387T/s3t3. What is the current in the loop (magnitude and direction) at the instant when B = 1.33 T?

Short Answer

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Step by step solution

01

Step 1:

Our target variable is the current in the loop at the instant B = 1.33 T. The direction of

the current is specified by Lenz's law. The magnitude of the current in the loop with

resistance R is given by

I= ε/R

Where ε, the induced emf, is given by Faraday's

law. We need to solve for the time at which B =1.33 T to evaluate

the induced emf and thus the current at this time.

By Lenz's law, the induced current must produce a magnetic fieldBinducedinside the loop that is upward, opposing the change in flux from the right-hand rule we described for the direction of the magnetic field produced by a circular loop Binduced, which will be in the desired direction if the induced current flows as shown in Fig. 1 in the

Counter clock-wise direction. The magnetic field is uniform over the loop and perpendicular to the plane of the loop, so the magnetic flux Binduced=BA,A=πr2is the area of the circular loop. Hence, by Faraday's law the induced a EMFs.

ε=-dΦBdt=-ddt(BA)=-AdBdt=-πr2dBdt

So, the magnitude of the current in the loop is

I=|ε|R=πr2RdBdt.

The time derivative of B is dB/dt=(1.14T/s3)t2so, we obtain

I=πr2R(1.14T/s3)t2

02

The time at a particular field.

The time t* corresponding to the field B = 1.33T satisfies the equation B(t*) =1.33T. Solving for t* gives

(0.380T/s3)(t*)3=1.33Tt*=1.33T0.380T/s3a=1.52s

Substitute this time and the known values of r and R into the expression for I gives

I=π(0.0250m)20.390Ω(1.14T/s3)(1.52s)2=13.3mA

Hence, the value of I is 13.3mA.

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